Abstract:We consider a 3×3 spectral problem which generates four-component CH type systems. The bi-Hamiltonian structure and infinitely many conserved quantities are constructed for the associated hierarchy. Some possible reductions are also studied.Mathematical Subject Classification: 37K10, 37K05
“…(2) the Hunter-Saxton equation [3,24] m t + m x u + 2mu x = 0, m = u xx , (1.4) (3) multicomponent generalizations of CH [8,18,19,27], for example the Geng-Xue (two-component) equation:…”
A spectral and the inverse spectral problem are studied for the two-component modified Camassa-Holm type for measures associated to interlacing peaks. It is shown that the spectral problem is equivalent to an inhomogenous string problem with Dirichlet/Neumann boundary conditions. The inverse problem is solved by Stieltjes's continued fraction expansion, leading to an explicit construction of peakon solutions. Sufficient conditions for global existence of solutions are given. The large time asymptotics reveals that, asymptotically, peakons pair up to form bound states moving with constant speeds. The peakon flow is shown to project to one of the isospectral flows of the finite Kac-van Moerbeke lattice. XIANG-KE CHANG, XING-BIAO HU, AND JACEK SZMIGIELSKI Appendix A. Lax pair for peakon ODEs 24 References 26
“…(2) the Hunter-Saxton equation [3,24] m t + m x u + 2mu x = 0, m = u xx , (1.4) (3) multicomponent generalizations of CH [8,18,19,27], for example the Geng-Xue (two-component) equation:…”
A spectral and the inverse spectral problem are studied for the two-component modified Camassa-Holm type for measures associated to interlacing peaks. It is shown that the spectral problem is equivalent to an inhomogenous string problem with Dirichlet/Neumann boundary conditions. The inverse problem is solved by Stieltjes's continued fraction expansion, leading to an explicit construction of peakon solutions. Sufficient conditions for global existence of solutions are given. The large time asymptotics reveals that, asymptotically, peakons pair up to form bound states moving with constant speeds. The peakon flow is shown to project to one of the isospectral flows of the finite Kac-van Moerbeke lattice. XIANG-KE CHANG, XING-BIAO HU, AND JACEK SZMIGIELSKI Appendix A. Lax pair for peakon ODEs 24 References 26
“…The first (4CH) system include as a special case the (3CH) system considered by Xia, Zhou and Qiao while the second contains the two-component generalizations of Novikov system considered by Geng and Xiu. Our Lax pair is a matrix generalization of the Lax pair for the four component Camassa-Holm type hierarchy considered in [32]. Our matrix Lax representation produces a huge number of different cubic CH type equations and it will be interesting to investigate these further, especially to study the existence of infinitely many conservation laws.…”
Two different four component Camassa-Holm (4CH) systems with cubic nonlinearity are proposed. The Lax pair and Hamiltonian structure are defined for both (CH) systems. The first (4CH) system include as a special case the (3CH) system considered by Xia, Zhou and Qiao, while the second contains the two-component generalization of Novikov system considered by Geng and Xiu.
“…As pointed out in Ref. [19], the three-component system (5) is the compatible condition of the spectral problem (4) and associated auxiliary problem…”
Abstractwe discuss a reciprocal transformation for a three-component Camassa-Holm type equation and find that the transformed system is a reduction of the first negative flow for an extended MKdV hierarchy.Mathematical Subject Classification: 37K10, 37K05
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